Can you explain why (at 1:05) the pressure forces act inwards as opposed to in the direction of flow / where in Chapter 2 specifically should I look to find out why?
@Tom-ts5qdКүн бұрын
Does this mean the Bernoulli Equation / Venturi effect can be applied to non ideal fluids as well? (approximately of course)
@FluidMatters22 сағат бұрын
Yes. In real (viscous) fluids there are some energy losses. But "Bernoulli" is often still a good approximation for air and water, which both have low viscosity.
@francisfrancis42192 күн бұрын
A submerged ball when released does not “rocket out of the water”. It rockets up when in the water, but only to reach the surface.
@jacobhardy23138 күн бұрын
Great video and explanation
@FluidMatters8 күн бұрын
Thanks. Glad to hear it was helpful.
@URKAEELIZACOLINPOWELL-ci1hw15 күн бұрын
Is it the no slip condition that causes the velocity gradient, professor or the internal shear stresses?
@FluidMatters13 күн бұрын
I'm not sure which part of this video you are specifically referring to. Here is a general answer. The fluid "sticks" to the surface i.e., the no slip condition. If the fluid above a stationary surface is moving (because of a pump or fan, for example), the fluid's viscosity will decrease (to zero) as you approach the surface. It's the internal viscous shear forces in the fluid, which opposes fluid motion, that slows the fluid in the near wall region. So, to answer your question, it is both effects. I hope that helps.
@URKAEELIZACOLINPOWELL-ci1hw13 күн бұрын
So, hypothetically speaking, even if there doesn't exist 'no-slip' at the bottom surface ( but the fluid sticks to the top surface) there would be a velocity gradient in the fluid, solely because of the internal friction between them. Am I right, professor?
@URKAEELIZACOLINPOWELL-ci1hw13 күн бұрын
I meant internal resistance between the fluid layers, alone, sir.
@user-pd5bn6qf5k15 күн бұрын
when you have losses, you add them to get to EGL?
@FluidMatters15 күн бұрын
Yes. The EGL remains constant only in the ideal friction case. But in the real world you always have energy losses in the flow direction. So, the EGL decreases because of energy losses (due to turbulence, wall viscous friction & pressure losses across a valve.) I hope that helps.
@ballerslounge285516 күн бұрын
Thanks for this lecture Dr Neylor i have a question though at 11:42 is the height difference not supposed to be (Z3 - Z2) or it doesnt matter
@FluidMatters13 күн бұрын
Note that z is measured upward, i.e. Z2>Z3. You need that term to be positive, since you are moving downward into zone of higher pressure. So it must be Z2-Z3 to get a positive number. You might find it easier to work in terms of DeltaZ, where DeltaZ is always a positive value.
@john-hf9dt18 күн бұрын
Thank you sir.
@antoniamillaraylizanaraban938020 күн бұрын
THIS VIDEO IS SO GOOD
@zhenccc22 күн бұрын
All your videos helped a lot. Thank you so much!
@javierpicazo210725 күн бұрын
I like this series
@Kawsusstory26 күн бұрын
Is that a plaquette on a hinge?
@Mehdiranjb29 күн бұрын
🌹🌹
@TerminallyOnline92Ай бұрын
At 13:29, shouldn’t it be C1 = -1/(2*mu*b)*dp/dx - U/b and not C1 = -b/(2*mu)*dp/dx - U/b ? Doing the algebra, I feel the b should be in the bottom of the fraction and not the top. Can someone explain please?
@FluidMattersАй бұрын
Before simplification, we have b^2 in the numerator (from y^2 in the original expression applied at b). So, when you divide by b to isolate C1, you end up with b in the numerator. I hope that helps.
@TerminallyOnline92Ай бұрын
@@FluidMattersThanks! I didn’t see that
@suleyman7478Ай бұрын
great stuff
@RGCADАй бұрын
Great stuff, for the last problem i see we have our origin placed midway between the plates, I would therefore expect the y at the bottom to be y = -h
@FluidMattersАй бұрын
Agree. The axis in the graphic (that I stole from the book publisher) is in the wrong place. But I think it's totally clear in the presentation that y=0 is at the bottom. At some point, a long time ago, I fixed it in the pdf download.
@baaa-ej7xjАй бұрын
He saved my final exam😭😭😭
@comment8767Ай бұрын
Point of Confusion for me - The cube as 6 faces with viscous stresses on each face. Therefore, there are 6 x 3 = 18 stresses on the differential element. Are we somehow saying that the stresses on opposite faces are the same, so that it is really only one? Then, all stresses are referred to a central point? What happens to the extra nine stresses?
@comment8767Ай бұрын
OK, so you are not claiming that the nine stresses cover the entire differential volume. You are simply positing the stresses on three faces, and then using taylor series to get the stresses on the opposite face. The posited stress plus the Taylor-derived stress provide the stress on the entire cube.
@mohammadfallahzade2110Ай бұрын
best instructor
@FluidMattersАй бұрын
Thanks for the kind words. Best of luck with your studies.
@mohammadfallahzade2110Ай бұрын
thank you you are a great teacher
@jamboreejackson8309Ай бұрын
Hi professor, many thanks for the excellent lectures. I tried the derivation of the equation in cylindrical co-ordinates and I couldn't quite get there so ended up looking at another reference. Should the dA in the outlet term you show at 14:30 actually be (r+dr)dΘdz (rather than rdΘdz) to account for the slightly larger area at the outer radius? This is what the derivation I saw suggested.
@FluidMattersАй бұрын
Good point. Yes, I think you are correct.
@mohammadfallahzade2110Ай бұрын
thank you for your great explanation
@spiral-dz1eqАй бұрын
from 3:40 on, why didn't we use the fluid for W and the wood for Fb?
@FluidMattersАй бұрын
As shown in the free body diagram, W is the weight of the WOOD and Fb is the buoyancy force. Thus, Fb is the weight of the WATER displaced by the wood (Archimedes principle). That is why I used the specific gravity of wood for W, and the specific gravity of water for Fb. I hope that helps.
@spiral-dz1eqАй бұрын
@@FluidMatters Thank you!
@andrewmerafuentes6683Ай бұрын
I came just to check for a concept, then proceed to finish the whole series.
@FluidMattersАй бұрын
Glad to be able to help. Best of luck with your studies.
@abdullahashraf8249Ай бұрын
what da dog doing
@rashedshahariar27482 ай бұрын
Where is the vertical force acting on the top of the free body in no 2 prblm 7:55
@FluidMatters2 ай бұрын
If I'm understanding your question: There is no vertical force on "the top of the free body". The vertical force acts upward and equals the weight of the water, which acts downward.
@rashedshahariar27482 ай бұрын
@@FluidMatters if we considered only the upper left quarter of the circle instead of the semi circle then there would have been vertical force acting on the upper part of the quarter circle then why not for the semi circle?
@rashedshahariar27482 ай бұрын
At 6:57 inclined forces at the upper portion should have vertical components ..isn't it? Can u pls clarify?
@gani822 ай бұрын
Continue the videos sir ..... following your videos ... ..waiting to learn from you sir.....
@FluidMatters2 ай бұрын
Glad to hear you find them helpful. Good luck with your studies.
@colinwarn46062 ай бұрын
Just wanted to extend my thanks for putting together a great KZbin series on Fluid Mechanics. Been a couple years since I've taken the class, the series has been a great refresher on the theory, in addition to tying it to some very informative experiments that visually cement the concepts 🙂
@FluidMatters2 ай бұрын
Thanks. Great to hear!
@anthonylorenzo11262 ай бұрын
Why isn't d^2u/dy^2 not 0?
@FluidMatters2 ай бұрын
d2u/dy2=0 means that the velocity profile must be linear i.e. no curvature. There is no basis for this requirement, as you can see from the solution.
@jondory81342 ай бұрын
Nice job... Related to the FBD, do you need to include a Moment, M, along with the Fx & Fy? (assume a direction...?)
@FluidMatters2 ай бұрын
This analysis is based on conservation of LINEAR momentum. So the are the forces needed to redirect the jet. No moment.
@KT-dv8qy2 ай бұрын
THANKS A LOT SIR!!!!
@FluidMatters2 ай бұрын
Glad to hear it was helpful. Best of luck with your studies.
@renatosureal2 ай бұрын
To estimate the impact force of a 5-meter fall from a 90 kg person, we can use the work-energy principle which states that the work done by the impact force is equal to the change in kinetic energy. When a person falls from a height, they gain kinetic energy, which is then absorbed by the impact. The kinetic energy (KE) just before impact is given by: $$ KE = \frac{1}{2} m v^2 $$ Where: - \( m \) is the mass (90 kg in this case), - \( v \) is the velocity at impact. The velocity at impact can be found using the equation for velocity of an object in free fall: $$ v = \sqrt{2gh} $$ Where: - \( g \) is the acceleration due to gravity (approximately \( 9.81 \, m/s^2 \)), - \( h \) is the height of the fall (5 meters). Substituting the values, we get: $$ v = \sqrt{2 \times 9.81 \, m/s^2 \times 5 \, m} $$ $$ v = \sqrt{98.1 \, m^2/s^2} $$ $$ v \approx 9.9 \, m/s $$ Now we can calculate the kinetic energy: $$ KE = \frac{1}{2} \times 90 \, kg \times (9.9 \, m/s)^2 $$ $$ KE = \frac{1}{2} \times 90 \, kg \times 98.01 \, m^2/s^2 $$ $$ KE = 4410.45 \, J $$ The impact force (F) can then be estimated if we know the distance over which the impact force acts (d), which is the distance over which the person's momentum is brought to zero. This distance will depend on many factors, including how the person lands and the nature of the surface they land on. Assuming a certain stopping distance, we can use the formula: $$ F = \frac{KE}{d} $$ For example, if the person comes to a stop over a distance of 0.5 meters, the impact force would be: $$ F = \frac{4410.45 \, J}{0.5 \, m} $$ $$ F = 8820.9 \, N $$ So the impact force would be approximately **8820.9 Newtons**. Please note that this is a simplified calculation and the actual impact force can vary. For accurate results, especially for safety considerations or engineering applications, a detailed analysis considering all relevant factors would be necessary. Source: Conversation with Bing, 4/30/2024 (1) Impact Force Calculator - Calculate the impact force in a collision. www.gigacalculator.com/calculators/impact-force-calculator.php. (2) Impact Force - The Engineering ToolBox. www.engineeringtoolbox.com/impact-force-d_1780.html. (3) Free Fall Force Calculator Online. calculatorshub.net/physics-calculators/free-fall-force-calculator/. (4) Impact Force Calculator | Calculate Impact Force in Collision .... physicscalc.com/physics/impact-force-calculator/. (5) Impact Energy Calculator | Impact Force. www.omnicalculator.com/physics/impact-energy.
@FluidMatters2 ай бұрын
ok
@ethanbaldwin11812 ай бұрын
Cool video!
@majroi2 ай бұрын
Greetings from Turkey, this material helped me a lot. Thanks professor.
@ericjung76212 ай бұрын
hi professor, why are there no videos for content past chapter 5?
@FluidMatters2 ай бұрын
That's where the intro fluid mechanics course ends at my university. I don't teach "Fluids II", at least for now.
@Frankchouzpy2 ай бұрын
Impressive profound experiment and explanation. Additionally, I encountered numerous novel ideas in the comments section here.
@FluidMatters2 ай бұрын
Thanks for the kind words. A colleague and I ended up writing a paper on this effect.
@Frankchouzpy2 ай бұрын
These interesting videos make your tutorial more and more attractive. These formulas jump out of the screen and appear in our lives. Thank you for your amazing idea!
@Frankchouzpy2 ай бұрын
Nice! Chapter 2 completed!!Next is the two ptional videos haha.
@Frankchouzpy2 ай бұрын
I can’t stop learning, so take a break, click the like button, and then continue!
@mfn13112 ай бұрын
why do I have a course called wave physics and fluid mechanics? I think both are hard enough on their own 🥲
@FluidMatters2 ай бұрын
Must be a different Dr. Naylor for the wave physics....
@salmankhanmohmand91742 ай бұрын
Sir where can i get its theory part...
@FluidMatters2 ай бұрын
Here's the theory lecture for hydrostatic forces on curved surfaces: kzbin.info/www/bejne/gpXFdqOIjbqjhbMsi=DoySt3zv_nYTipHn You can find all the lectures as www.drdavidnaylor.net
@AtroXAir2 ай бұрын
Great explanation! thank you very much
@Frankchouzpy2 ай бұрын
Thanks for your great work on this playlist!!! I have learnt much from it. But there seems to be an integrate error at 21:45, the relationship of the p and p0 should include some exp. function or Ln function after the integration. Please check it. You have done such an excellent tutorial which is so useful for a student who is interested in the fluid mechanics! Thank you agian from China.
@FluidMatters2 ай бұрын
The integration is correct. Notice there "z" in the dominator on the left side too (the adiabatic lapse rate). So, you get "ln" function on both sides. So, you end up taking the anti-log of both sides, after integration. The final results is a well-know equation -- you can just google Standard Atmosphere Equation, and you will find it is correct.
@Frankchouzpy2 ай бұрын
@@FluidMatters Oh, I made a mistake. I didn't realize that the integrand on the left is the reciprocal of p instead of 1. I apologize for rushing my question, and thank you very much for your answer. Your tutorial is excellent, just like you. Bravo!
@batbayarbatsukh63932 ай бұрын
Greetings from Mongolia. Thanks for the clear explanation. Тhis helped me a lot I wish you good health.
@FluidMatters2 ай бұрын
Mongolia! Hope to visit one day. Glad to hear the video was helpful.
@alisoltani75812 ай бұрын
Hello , what about the unsteady case? how can we sole this problem for u(t,y)?
@FluidMatters2 ай бұрын
There are exact solutions for some simple unsteady problems, like an impulsively accelerated plane wall. This is beyond the undergrad level. See the classic book "Boundary-Layer Theory" by Schlichting, for example.
@alisoltani75812 ай бұрын
@@FluidMatters Ok,thank you very much🙏🙏
@Frankchouzpy2 ай бұрын
Nice work thx. from China!😘
@schwarzehayvan81882 ай бұрын
Great Videos and Work. Thank you from Germany
@FluidMatters2 ай бұрын
Glad you like them!
@masoudadli1083 ай бұрын
the best of the best,, you make life easy..thanks from Sudan Africa
@FluidMatters3 ай бұрын
Thanks for the kind words. Glad to hear the videos are helpful.
@lucasdovale92933 ай бұрын
Nice climb dude, those slabs look hard. Also, i was very happy to see both my hobbies in the channel, fluid mechanics and climbing!